-
2
-
-
0001908290
-
-
F.T. Arecchi et al, Phys. Rep.10.1016/S0370-1573(99)00007-1 318, 1 (1999).
-
(1999)
Phys. Rep.
, vol.318
, pp. 1
-
-
Arecchi, F.T.1
-
4
-
-
0001219206
-
-
K. Staliunas et al, Phys. Rev. A10.1103/PhysRevA.51.4140 51, 4140 (1995);
-
(1995)
Phys. Rev. A
, vol.51
, pp. 4140
-
-
Staliunas, K.1
-
6
-
-
0028386874
-
-
G.L. Oppo et al, Phys. Rev. A10.1103/PhysRevA.49.2028 49, 2028 (1994);
-
(1994)
Phys. Rev. A
, vol.49
, pp. 2028
-
-
Oppo, G.L.1
-
7
-
-
0000130310
-
-
S.J. Jensen et al, Phys. Rev. Lett.10.1103/PhysRevLett.81.1614 81, 1614 (1998).
-
(1998)
Phys. Rev. Lett.
, vol.81
, pp. 1614
-
-
Jensen, S.J.1
-
8
-
-
84957315501
-
-
W.J. Firth and A.J. Scroggie, Europhys. Lett. 26, 521 (1994);
-
(1994)
Europhys. Lett.
, vol.26
, pp. 521
-
-
-
9
-
-
0030568352
-
-
W.J. FirthA.J. ScroggiePhys. Rev. Lett.10.1103/PhysRevLett.76.1623 76, 1623 (1996).
-
(1996)
Phys. Rev. Lett.
, vol.76
, pp. 1623
-
-
-
13
-
-
0028403825
-
-
For cross-phase modulation in a cavity, two fields of orthogonal polarizations, each having its own resonant frequencies, interact through (Formula presented). In contrast to our case, for each polarization (separately) the interference between beams from different cycles critically contributes to (Formula presented). See M. Haelterman et al, J. Opt. Soc. Am. B 11, 446 (1994).
-
(1994)
J. Opt. Soc. Am. B
, vol.11
, pp. 446
-
-
Haelterman, M.1
-
15
-
-
0346876660
-
-
M. Soljacic et al, Phys. Rev. Lett.10.1103/PhysRevLett.84.467 84, 467 (2000);
-
(2000)
Phys. Rev. Lett.
, vol.84
, pp. 467
-
-
Soljacic, M.1
-
16
-
-
0033761260
-
-
D. Kip et al, Science10.1126/science.290.5491.495 290, 495 (2000).
-
(2000)
Science
, vol.290
, pp. 495
-
-
Kip, D.1
-
18
-
-
85038282231
-
-
Near and above the threshold, our approximations fail. Relaxing (Formula presented) adds “second-order MI,” where higher harmonics of the dominant frequency considerably increase the visibility of the pattern—just as we observe experimentally. Including the contributions of beams that circulate more than once does not change the features but skews the threshold value
-
Near and above the threshold, our approximations fail. Relaxing (Formula presented) adds “second-order MI,” where higher harmonics of the dominant frequency considerably increase the visibility of the pattern—just as we observe experimentally. Including the contributions of beams that circulate more than once does not change the features but skews the threshold value.
-
-
-
-
19
-
-
3342975405
-
-
M. Segev et al, Phys. Rev. Lett.10.1103/PhysRevLett.73.3211 73, 3211 (1994);
-
(1994)
Phys. Rev. Lett.
, vol.73
, pp. 3211
-
-
Segev, M.1
-
21
-
-
79957775841
-
-
M. Shih et al, Electron. Lett.10.1049/el:19950570. 31, 826 (1995).
-
(1995)
Electron. Lett.
, vol.31
, pp. 826
-
-
Shih, M.1
-
22
-
-
39249083623
-
-
Unit conversion is as in T. Carmon et al, Phys. Rev. Lett.10.1103/PhysRevLett.87.143901 87, 143901 (2001).
-
(2001)
Phys. Rev. Lett.
, vol.87
, pp. 143901
-
-
Carmon, T.1
-
23
-
-
0000054909
-
-
S. Ducci et al, Phys. Rev. Lett.10.1103/PhysRevLett.83.5210 83, 5210 (1999).
-
(1999)
Phys. Rev. Lett.
, vol.83
, pp. 5210
-
-
Ducci, S.1
-
24
-
-
0029637529
-
-
D. Engin et al, Phys. Rev. Lett.10.1103/PhysRevLett.74.1743 74, 1743 (1995);
-
(1995)
Phys. Rev. Lett.
, vol.74
, pp. 1743
-
-
Engin, D.1
-
25
-
-
0000448194
-
-
S.G. Odoulov et al, Phys. Rev. Lett.10.1103/PhysRevLett.83.3637 83, 3637 (1999).
-
(1999)
Phys. Rev. Lett.
, vol.83
, pp. 3637
-
-
Odoulov, S.G.1
-
28
-
-
0000725128
-
-
O. Zik et al, Phys. Rev. Lett.10.1103/PhysRevLett.73.644 73, 644 (1994).
-
(1994)
Phys. Rev. Lett.
, vol.73
, pp. 644
-
-
Zik, O.1
|